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Segal's axioms and bootstrap for Liouville Theory

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arxiv 2112.14859 v2 pith:3AJVD3SZ submitted 2021-12-29 math.PR math-phmath.CVmath.MPmath.RT

classification math.PRmath-phmath.CVmath.MPmath.RT
keywords conformalsegalfunctionslcftstructuretheoryaxiomscalled
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In 1987 Graeme Segal gave a functorial definition of Conformal Field Theory (CFT) that was designed to capture the mathematical essence of the Conformal Bootstrap formalism pioneered in physics by Belavin-Polyakov-Zamolodchikov. In Segal's formulation the basic objects of CFT, the correlation functions of conformal primary fields, are viewed as functions on the moduli space of Riemann surfaces with marked points which behave naturally under gluing of surfaces. In this paper we give a probabilistic realization of Segal's axioms in Liouville Conformal Field Theory (LCFT) which is a CFT that plays a fundamental role in the theory of random surfaces and two dimensional quantum gravity. Then we use Segal's axioms to express the correlation functions of LCFT in terms of the basic objects of LCFT: its {\it spectrum} and its {\it structure constants}, determined in earlier works by the authors. As a consequence, we obtain a formula for the correlation functions as multiple integrals over the spectrum of LCFT, the structure of these integrals being associated to a pant decomposition of the surface. The integrand is the modulus squared of a function called conformal block: its structure is encoded by the commutation relations of an algebra of operators called the Virasoro algebra and it depends holomorphically on the moduli of the surface with marked points. The integration measure involves a product of structure constants, which have an explicit expression, the so called DOZZ formula.

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Cited by 3 Pith papers

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  1. Probabilistic construction of non compactified imaginary Liouville field theory

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    A path integral over a real Gaussian free field with a Hankel-contour zero mode reproduces the imaginary DOZZ three-point function without a neutrality condition.

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    A ratio of partition functions on branched covers, defined by Cauchy-Hadamard renormalization, transforms under Weyl rescalings exactly as twist-field correlation functions with weights Δ_j = (c/12) Σ (1 - 1/ord_f(z)).

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